拓扑$mathrm{K}$理论的实自旋边界和定向

Zachary Halladay, Yigal Kamel
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摘要

我们构建了一个交换正交$C_2$环谱,$mathrm{MSpin}^c_{math/bb{R}}$,以及一个$C_2$-$E_{infty}$-orientation$mathrm{MSpin}^c_{math/bb{R}}$。\到阿蒂亚实科理论的 \mathrm{KU}_{mathbb{R}}$。此外,我们定义 $E_{\infty}$ 映射 $\mathrm{MSpin}\to(\mathrm{MSpin}^c_{\mathbb{R}})^{C_2}$ and $\mathrm{MU}_{\mathbb{R}}用来恢复拓扑 $\mathrm{K}$ 理论的三个著名定向:$\mathrm{MSpin}^c \to\mathrm{KU}$ 、$\mathrm{MSpin}^c \to\mathrm{KU}$ 、$\mathrm{MSpin}^c \to\mathrm{KU}$ 和$\mathrm{MSpin}^c \to\mathrm{KU}$ 。\從映射 $\mathrm{MSpin}^c_{\mathbb{R}} 到 $\mathrm{MU}_{\mathbb{R}} 到 $\mathrm{KU}_{\mathbb{R}}$, 从映射 $\mathrm{MSpin}^c_{\mathbb{R}}\to\mathrm{KU}_{\mathbb{R}}$.我们还利用$underline{pi}_*\mathrm{MSpin}^c_{mathbb{R}} 的麦基函子结构证明了自旋流形上$\hat{A}$-元的积分性为定点$(\mathrm{MSpin}^c_{mathbb{R}})^{C_2}$等价于$\mathrm{MSpin}$提供了障碍。特别是,通常的映射 $\mathrm{MSpin}\到 \mathrm{MSpin}^c$的通常映射不会作为任何$C_2$-$E_{\infty}$环谱的定点包含而出现。
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Real spin bordism and orientations of topological $\mathrm{K}$-theory
We construct a commutative orthogonal $C_2$-ring spectrum, $\mathrm{MSpin}^c_{\mathbb{R}}$, along with a $C_2$-$E_{\infty}$-orientation $\mathrm{MSpin}^c_{\mathbb{R}} \to \mathrm{KU}_{\mathbb{R}}$ of Atiyah's Real K-theory. Further, we define $E_{\infty}$-maps $\mathrm{MSpin} \to (\mathrm{MSpin}^c_{\mathbb{R}})^{C_2}$ and $\mathrm{MU}_{\mathbb{R}} \to \mathrm{MSpin}^c_{\mathbb{R}}$, which are used to recover the three well-known orientations of topological $\mathrm{K}$-theory, $\mathrm{MSpin}^c \to \mathrm{KU}$, $\mathrm{MSpin} \to \mathrm{KO}$, and $\mathrm{MU}_{\mathbb{R}} \to \mathrm{KU}_{\mathbb{R}}$, from the map $\mathrm{MSpin}^c_{\mathbb{R}} \to \mathrm{KU}_{\mathbb{R}}$. We also show that the integrality of the $\hat{A}$-genus on spin manifolds provides an obstruction for the fixed points $(\mathrm{MSpin}^c_{\mathbb{R}})^{C_2}$ to be equivalent to $\mathrm{MSpin}$, using the Mackey functor structure of $\underline{\pi}_*\mathrm{MSpin}^c_{\mathbb{R}}$. In particular, the usual map $\mathrm{MSpin} \to \mathrm{MSpin}^c$ does not arise as the inclusion of fixed points for any $C_2$-$E_{\infty}$-ring spectrum.
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